<p>Let <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\(\mathcal {R}=\mathbb {F}_{q^2}+\mu \mathbb {F}_{q^2}+\nu \mathbb {F}_{q^2}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi mathvariant="script">R</mi> <mo>=</mo> <msub> <mi mathvariant="double-struck">F</mi> <msup> <mi>q</mi> <mn>2</mn> </msup> </msub> <mo>+</mo> <mi>μ</mi> <msub> <mi mathvariant="double-struck">F</mi> <msup> <mi>q</mi> <mn>2</mn> </msup> </msub> <mo>+</mo> <mi>ν</mi> <msub> <mi mathvariant="double-struck">F</mi> <msup> <mi>q</mi> <mn>2</mn> </msup> </msub> </mrow> </math></EquationSource> </InlineEquation>, where <i>q</i> is a prime power, <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(\mu ^2=\mu \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msup> <mi>μ</mi> <mn>2</mn> </msup> <mo>=</mo> <mi>μ</mi> </mrow> </math></EquationSource> </InlineEquation>, <InlineEquation ID="IEq6"> <EquationSource Format="TEX">\(\nu ^2=\nu \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msup> <mi>ν</mi> <mn>2</mn> </msup> <mo>=</mo> <mi>ν</mi> </mrow> </math></EquationSource> </InlineEquation> and <InlineEquation ID="IEq7"> <EquationSource Format="TEX">\(\mu \nu =\nu \mu =0\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>μ</mi> <mi>ν</mi> <mo>=</mo> <mi>ν</mi> <mi>μ</mi> <mo>=</mo> <mn>0</mn> </mrow> </math></EquationSource> </InlineEquation>. In this paper, we study the structural properties of skew <InlineEquation ID="IEq8"> <EquationSource Format="TEX">\(\lambda \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>λ</mi> </math></EquationSource> </InlineEquation>-constacyclic codes over <InlineEquation ID="IEq9"> <EquationSource Format="TEX">\(\mathbb {F}_{q^2}\mathcal {R}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi mathvariant="double-struck">F</mi> <msup> <mi>q</mi> <mn>2</mn> </msup> </msub> <mi mathvariant="script">R</mi> </mrow> </math></EquationSource> </InlineEquation>, where <InlineEquation ID="IEq10"> <EquationSource Format="TEX">\(\lambda \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>λ</mi> </math></EquationSource> </InlineEquation> is a unit of <InlineEquation ID="IEq11"> <EquationSource Format="TEX">\(\mathcal {R}\)</EquationSource> <EquationSource Format="MATHML"><math> <mi mathvariant="script">R</mi> </math></EquationSource> </InlineEquation>. Define a Gray map <InlineEquation ID="IEq12"> <EquationSource Format="TEX">\(\varPhi \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>Φ</mi> </math></EquationSource> </InlineEquation> from <InlineEquation ID="IEq13"> <EquationSource Format="TEX">\(\mathbb {F}_{q^2}^{\alpha }\times \mathcal {R}^{\beta }\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msubsup> <mi mathvariant="double-struck">F</mi> <mrow> <msup> <mi>q</mi> <mn>2</mn> </msup> </mrow> <mi>α</mi> </msubsup> <mo>×</mo> <msup> <mrow> <mi mathvariant="script">R</mi> </mrow> <mi>β</mi> </msup> </mrow> </math></EquationSource> </InlineEquation> to <InlineEquation ID="IEq14"> <EquationSource Format="TEX">\(\mathbb {F}_{q^2}^{\alpha +3\beta }\)</EquationSource> <EquationSource Format="MATHML"><math> <msubsup> <mi mathvariant="double-struck">F</mi> <mrow> <msup> <mi>q</mi> <mn>2</mn> </msup> </mrow> <mrow> <mi>α</mi> <mo>+</mo> <mn>3</mn> <mi>β</mi> </mrow> </msubsup> </math></EquationSource> </InlineEquation> preserving the Hermitian orthogonality, where <InlineEquation ID="IEq15"> <EquationSource Format="TEX">\(\alpha \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>α</mi> </math></EquationSource> </InlineEquation> and <InlineEquation ID="IEq16"> <EquationSource Format="TEX">\(\beta \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>β</mi> </math></EquationSource> </InlineEquation> are positive integers. Furthermore, we give a necessary and sufficient condition for skew <InlineEquation ID="IEq17"> <EquationSource Format="TEX">\(\lambda \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>λ</mi> </math></EquationSource> </InlineEquation>-constacyclic codes over <InlineEquation ID="IEq18"> <EquationSource Format="TEX">\(\mathbb {F}_{q^2}\mathcal {R}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi mathvariant="double-struck">F</mi> <msup> <mi>q</mi> <mn>2</mn> </msup> </msub> <mi mathvariant="script">R</mi> </mrow> </math></EquationSource> </InlineEquation> to be linear complementary dual (LCD). Then we obtain some LCD codes as the <InlineEquation ID="IEq19"> <EquationSource Format="TEX">\(\varPhi \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>Φ</mi> </math></EquationSource> </InlineEquation>-images of Hermitian LCD skew <InlineEquation ID="IEq20"> <EquationSource Format="TEX">\(\lambda \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>λ</mi> </math></EquationSource> </InlineEquation>-constacyclic codes. We also enumerate the Hermitian LCD skew <InlineEquation ID="IEq21"> <EquationSource Format="TEX">\(\lambda \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>λ</mi> </math></EquationSource> </InlineEquation>-constacyclic codes over <InlineEquation ID="IEq22"> <EquationSource Format="TEX">\(\mathcal {R}\)</EquationSource> <EquationSource Format="MATHML"><math> <mi mathvariant="script">R</mi> </math></EquationSource> </InlineEquation>. Finally, based on the study of Hermitian LCD skew <InlineEquation ID="IEq23"> <EquationSource Format="TEX">\(\lambda \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>λ</mi> </math></EquationSource> </InlineEquation>-constacyclic codes over <InlineEquation ID="IEq24"> <EquationSource Format="TEX">\(\mathbb {F}_{q^2}\mathcal {R}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi mathvariant="double-struck">F</mi> <msup> <mi>q</mi> <mn>2</mn> </msup> </msub> <mi mathvariant="script">R</mi> </mrow> </math></EquationSource> </InlineEquation>, we employ the Gray map to construct entanglement-assisted quantum error-correcting codes (EAQECCs) with the maximal entanglement.</p>

错误:搜索内容不能为空,请输入英文关键词
错误:关键词超出字数限制,请精简
高级检索

Lcd skew constacyclic codes over \(\mathbb {F}_{q^2}{\mathcal {R}}\) and their applications to EAQECCs

  • Zecheng Xu,
  • Fanghui Ma,
  • Jian Gao,
  • Juan Li

摘要

Let \(\mathcal {R}=\mathbb {F}_{q^2}+\mu \mathbb {F}_{q^2}+\nu \mathbb {F}_{q^2}\) R = F q 2 + μ F q 2 + ν F q 2 , where q is a prime power, \(\mu ^2=\mu \) μ 2 = μ , \(\nu ^2=\nu \) ν 2 = ν and \(\mu \nu =\nu \mu =0\) μ ν = ν μ = 0 . In this paper, we study the structural properties of skew \(\lambda \) λ -constacyclic codes over \(\mathbb {F}_{q^2}\mathcal {R}\) F q 2 R , where \(\lambda \) λ is a unit of \(\mathcal {R}\) R . Define a Gray map \(\varPhi \) Φ from \(\mathbb {F}_{q^2}^{\alpha }\times \mathcal {R}^{\beta }\) F q 2 α × R β to \(\mathbb {F}_{q^2}^{\alpha +3\beta }\) F q 2 α + 3 β preserving the Hermitian orthogonality, where \(\alpha \) α and \(\beta \) β are positive integers. Furthermore, we give a necessary and sufficient condition for skew \(\lambda \) λ -constacyclic codes over \(\mathbb {F}_{q^2}\mathcal {R}\) F q 2 R to be linear complementary dual (LCD). Then we obtain some LCD codes as the \(\varPhi \) Φ -images of Hermitian LCD skew \(\lambda \) λ -constacyclic codes. We also enumerate the Hermitian LCD skew \(\lambda \) λ -constacyclic codes over \(\mathcal {R}\) R . Finally, based on the study of Hermitian LCD skew \(\lambda \) λ -constacyclic codes over \(\mathbb {F}_{q^2}\mathcal {R}\) F q 2 R , we employ the Gray map to construct entanglement-assisted quantum error-correcting codes (EAQECCs) with the maximal entanglement.